non-reactive interaction of molecules with a surface: periodic or...
TRANSCRIPT
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St Petersburg – 16/09/2013
Non-reactive interaction of molecules with a
surface: periodic or cluster approach?
Marie GUITOU
Laboratoire MSME, Theoretical Chemistry
Université Paris-Est Marne-la-Vallée, France
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Molecule – surface interactions
Molecule/Surface
Surface catalysis
storagein solid Astrophysics :
gas/solid interaction
Spectroscopy
reaction
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Several interaction domains
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Several steps in the interaction process
I
II
III
Physisorption
Dissociation
Interaction energy of furtherlayers
Physisorption of further molecules
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PHYSISORPTION
CHEMISORPTIONDissociative
vdW
Choice of the computational method
Densityfunctional
Theory DFT
××××Periodic
OK�MCSCF�MRCI
�CCSD(T)
Cluster representation
Possible but difficult !
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Some aspects of the periodic (Slab) model
for the physisorption
The generally used method is DFT with various functionnalsamong which : PBE, PBEsol (especially adapted to solids), + eventually Grimme correction for long range interactions.
Different choices for the electronic calculation:- Plane waves for the electron description – code VASP- Localized atomic orbitals for the electrons – code CRYSTAL,this is preferred for molecular processus.
Appropriate choice of the unit cells for the periodic representation
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Periodic – Slab model of the surface
Definition of the unit cells for the periodic representation: different sizes of cell and 3 layers for the Slab
Cell 1 Cell 2
Cell 3
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Details of the periodic calculation (cell 3)
Coordinate system (X,Y,Z,θ,ϕ),Including lateral displacementsdH-H is fixed
Cu/Ag (n-1)s2(n-1)p6(n-1)d10ns1
-Grey atoms : all electrons calculation-Blue atoms : pseudopotentiel with 19explicit electrons
VASP or CRYSTAL
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A cluster to model the surface (constraints)
y
z
x Surface X(100)
(9,4,9)
Cu/Ag (n-1)s2(n-1)p6(n-1)d10ns1
Pseudopotentiel with 19 explicitelectrons for the central atomsPseudopotentiels with 1 explicit
electron for the outer atoms
Representation of the metallic (100) surface by a cluster composedof 22 atoms in 3 layers (9,4,9)
Advantage: Z- symmetryno artificial polarisation (µz=0)
Main concerns : Size - big enough cluster to be representativeLimit the border effects - consider the central part of the cluster
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Cluster Cu22/Ag22 and H2
Coordinate system, (Z,θ,ϕ),no lateral displacement,dH-H is fixed
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Parallel approaches Perpendicular approach
H2 in btbBridge-top-bridgeθ =90° Φ =0°
Several investigated geometries
H2 in hthhollow-top-hollowθ =90° Φ =45°
H2 in topθ =0° Φ =0°
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Physisorption
Shape of the Potential Energy
Surface
First layer interaction of H2 with
the (100) Ag surface of CFC
Periodic model
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Periodic (DFT) results obtained with CRYSTAL,
cell-3, PBEsol, rotations θRotation of H2 from vertical T⊥to parallel HTH to the surface, V (Z,θ), ϕ=45
T⊥ HTH
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Periodic (DFT) results obtained with CRYSTAL,
cell-3, PBEsol, rotations θ
Rotating the H2 from vertical T⊥to parallel BTB to the surface, V (Z,θ), ϕ=0
T⊥ BTB
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Periodic (DFT) results obtained with CRYSTAL, for
H2 on top of a metallic atom
Main results for the centre of mass of H2 positionned on top of a metallic atom:
1) The more stable position corresponds to the perpendicular T⊥approach, in good agreement withthe values of the polarisabilities of H2
α⊥ = 4,84 αơ = 6,30
αơ /α⊥=1,30 ET/EBTB = 1,33
2) The rotation with ϕ is almost isotropicfor the parallel positions (BTB and HTH)
T⊥ BTB HTH
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Periodic (DFT) results obtained with CRYSTAL, cell-
3, PBEsol, translations of perpendicular H2
For H2 perpendicular to the surface on top of various sites: Top T, Hollow H, Bridge B and intermediate ones.
The more metallic atoms are involved, the stronger is the interaction.
T⊥B⊥
H⊥
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Periodic (DFT) results obtained with CRYSTAL, cell-
3, PBEsol, translations of parallel positions
For H2 parallel to the surface on top of various sites: Top T, Hollow H, Bridge B and intermediate ones.
The more stable situations correspond to positions of the center ofmass of H2 on top of a metallic atom.
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Comparison of periodic (DFT) results obtained with
CRYSTAL and cluster model (MRCI) H2@Ag(100)
Exp: diffusion of H2 molecules on Ag surface(111)
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Comparison of the results with CRYSTAL and VASP
CRYSTAL VASP
VASP, with plane waves, canprovide comparable resultswith CRYSTAL when usingPBE + Grimme correction.
CRYSTAL seems more appropriate
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Physisorption, chemisorption
First layer interaction of H2 with
the (100) Cu surface
Cluster model
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Physisorption well requires longer range with Cu than with Ag
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(x, y, Z) : Centre of mass H2r ═ rHH : distance H-Hθ : angle (H-H / axe Z)Φ : angle (H-H / axe X)
H atom
Cu atom
Parameters of H2/surface system
(9,4,9)
MRCI+Q, CCSD(T), DFT
Molpro version 2010 : H.-J. Werner et P. Knowles ww w.tc.bham.ac.uk/molpro
),,,,,(2
1)(
162
2
2
2
2
2
2
2
2
φθµ HHDrot
HHH
ryxZVHryxZM
H ++∂
∂−∂∂+
∂∂+
∂∂−=
Surface (100)
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Physisorption energy of H2@Cu
CCSD(T) Ep (meV) Zp (Å)
top - 45.0 4.0
btb -8.0 4.5
hth -7.9 4.6
Z
Z
Ep= Emin - Eref
H-H distance remains at 0.74ÅEexp ~ -31 meV, Andersson et al, RPB 1988 ααααpara(H2)>ααααperp (H2)
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Barrier and Chemisorption energies H2@Cu
Approach BTB HTH
Method MRCI +Q CCSD(T) DFT* CCSD(T)
Barrier Z = 1.3 År (H-H)= 0.80 Å
E = 0.6 eV
Z = 1.4 År (H-H)= 0.80 Å
E = 0.4 eV
Z = 1.8 År (H-H)= 0.80 Å
E = 0.3 eV
Chemisorption
Z = 1.0 År (H-H)= 2.5 ÅE = -0.4 eV
Z = 1.0 År (H-H)= 2.5 ÅE = -0.5 eV
Z = 1.0 År (H-H)= 2.5 Å
E = -0.9eV (B3LYP)E = -1.0eV (PBE0)
E = -0.47eV (WB97XD)
Z = 0.3 År (H-H)= 3.1 ÅE = -0.7 eV
*19/1 pseudo19/19 E = - 0.27 eV
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Delocalisation correction by
embedding the cluster
Physisorption, barrier,
chemisorption
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Embedded cluster into a periodic system
EHL/LH = EHL(cluster) – ELL(cluster) +ELL(Slab)
To correct for the delocalization effect in themetal the cluster is embedded in a periodicsystem. ONIOM Method
Periodic code VASP:-Low level calculation (LL) DFT (PBE).-High level calculation CCSD(T) or MRCI+Q- In the slab calculation the unit cell is definedby the 22 atoms cluster surrounded by 5 layers of copper atoms..
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2D Potential energies V(Z,rHH), parallel approach
MRCI surface ONIOM surface
physisorption
chemisorptionbarrier
- Chemisorption well deeper with ONIOM (-0.05 eV)-Higher barrier with ONIOM (+0.21 eV)-No reliable access to the physisorption region
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Checking the accuracy of the
physisorption well
-------
Rotational spectroscopy of
physisorbed H2@Cu
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The H2 molecule centre-of-mass is constrained on the Z axis , on top of thecentral Cu atom. An accurate description of the 4D interaction potentialV(Z,r,θ,ϕ) is obtained with CCSD(T) calculation.
The rH-H parameter can be fixed at theequilibrium geometry of H2 molecule for large Z values. H2 is considered as a rigid rotor.
The variations of V with the angle φ arevery small (<1cm-1) and are neglected.
The potential is strongly anharmonic andanisotropic with respect to Z and θvariables.
Framework of the spectroscopic treatment
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The motion of H2 on the surface can thus be solved with a 2D Hamiltonian, where the motion associated with the angle φ - helicopter rotation above thesurface – is represented by the quantum number m, a ‘good’ quantum number.
Equation of the motion of the H2 molecule
Spectroscopic wavefunctions are represented, for the rotational motion,with associated Legendre functions, labelled with m.
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Expansion of the V2D(Z,θθθθ) potentialin the physisorption region
Analytic expansion of the van der Waals Z dependent term, developedin Morse type coordinate series
with
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Contour plot of the V2D(Z,θθθθ) potentialin the physisorption well
Z
Distance between lines equals 2.5 meV = 20cm-1
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Energies (in cm-1) of the first ro-vibrational levels(v for stretching, j for rotation θθθθ, and m for φφφφ)
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2 3 4 5 6 7 8 9 100
20
40
60
80
100
120
140
160
180
(000)
2 3 4 5 6 7 8 9 100
20
40
60
80
100
120
140
160
180
(100)
2 3 4 5 6 7 8 9 100
20
40
60
80
100
120
140
160
180
(010)
2 3 4 5 6 7 8 9 100
20
40
60
80
100
120
140
160
180
(110)
Contour plots of ro-vibrational wavefunctionsm=0, no-helicopter rotation of H2
E=239 cm-1 E=289 cm-1
E=303 cm-1 E=364 cm-1
θ
Z
Z
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2 3 4 5 6 7 8 9 100
20
40
60
80
100
120
140
160
180
(121)
2 3 4 5 6 7 8 9 100
20
40
60
80
100
120
140
160
180
(021)
Contour plots of ro-vibrational wavefunctions
m=1, including helicopter rotation of H2
E=601cm-1 E=650 cm-1
Z
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Comparison calculation/experiment
Transition Ecal (meV) Eexp (meV)
(000)→(021) 44 44
(000)→(121) 51 52
(000)→(221) 56 58
Measurements of Electron-Energy-LossSpectroscopy EELS, on Cu(100) surface,showing j=0→2 rotational transitions
in H2
Conditions : 10-11 Torr and T~10K. 3eV electron beam
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�It is still a challenge to have a full description of the interaction of a molecule with a surface for all distances within one given method. So far, with DFT methods, nofunctional is able to cover the whole range of distances and the long distances are difficult to obtain when metals are involved
�Short and intermediate range, interesting for reactivity on surface and catalysis, canbe described with periodic approaches or cluster representation with embeddingcorrection for more accurate description of the processes.
�Long range interaction, needed for non reactive dynamics on surfaces, multilayersproblems, nano-fluidic etc.., can be approached by cluster representation using highlycorrelated wavefunctions. Spectroscopy can be a good tool to check the performance of the techniques.
Conclusions
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Acknowledgments
� MLV:� Eddy Bernard� Céline Houriez� Sacha Mitrushchenkov� Gilberte Chambaud
� ENS Lyon� Florian Göltl� Philippe Sautet
� Herzen University
� Univ. Marne La Vallée� CNRS
� ANR DYQUMA
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Second layer interaction of H2
with the Cu (100) surface
Physisorption
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Polarisation of the surface by
chemisorbed H2
µZ= 3.1 Debye
Polarisation of surface atoms
Dipole moment along the Z axis
z
δ+
δ-
(MRCI)
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Physisorption H2/H-H-Cu(100)
CCSD(T) Parallèle BTB Perpendicul
E (meV) -24.4(-8)*
-20.7(-8)*
-68.6(-45)*
Z (Å) 3.9(4.5)*
4.0(4.5)*
3.7(4.0)*
[1] C. Houriez, E. Bernard, F. Göltl, Ph. Sautet, M . Guitou et G. Chambaud (RCTF – Marseille, 07 – 2012)
*Physisorption of the first layerFirst H 2 molecule fixed at the btb minimumLarger interaction in the second layer, closer approac h